TECHNICAL FIELD
[0001] The present invention relates to a a magnetic memory element, use and manufacturing
methods thereof, and particularly to a magnetic memory element operable as a magnetic
nonvolatile memory element, the use in a magnetic memory device composed of the magnetic
memory element and manufacturing methods thereof.
BACKGROUND ART
[0002] As information communication devices, in particular, personal small devices such
as personal digital assistants are making great spread, elements such as memories
and logics comprising information communication device are requested to have higher
performance such as higher integration degree, higher operation speed and lower power
consumption. In particular, technologies for making nonvolatile memories become higher
in density and larger in storage capacity are progressively increasing their importance
as technologies for replacing hard disk and optical disc that cannot be essentially
miniaturized because they have movable portions.
[0003] As nonvolatile memories, there may be enumerated flash memories using semiconductors
and FRAM (Ferro electric Random Access Memory) using ferroelectric material and the
like.
[0004] However, the flash memory encounters with a drawback that its write speed is as slow
as the microsecond order.
[0005] On the other hand, it is pointed out that the FRAM has a problem in which it cannot
be rewritten so many times.
[0007] Since this MRAM is simple in structure, it can easily be integrated at a higher integration
degree. Moreover, since it is able to memorize information based upon the rotation
of magnetic moment, it can be rewritten so many times. It is also expected that the
access time of this magnetic random access memory will be very high, and it was already
confirmed that it can be operated at the access time of nanosecond order.
[0008] A magnetoresistive effect element for use with this MRAM, in particular, a tunnel
magnetoresistive (Tunnel Magnetoresistance) element is fundamentally composed of a
lamination layer structure of a ferromagnetic tunnel junction of ferromagnetic layer/tunnel
barrier layer/ferromagnetic layer.
[0009] This element generates magnetoresistive effect in response to a relative angle between
the magnetizations of the two magnetic layers when an external magnetic field is applied
to the ferromagnetic layers under the condition in which a constant current is flowing
through the ferromagnetic layers. To be concrete, when the magnetization directions
of the two magnetic layers are anti-parallel to each other, a resistance value is
maximized. When they are parallel to each other, a resistance value is minimized.
Function of memory element can be demonstrated by creating the anti-parallel state
and the parallel state with application of the external magnetic field when the magnetization
direction of one ferromagnetic layer is inverted.
[0010] This resistance changing ratio is expressed by the following equation (1) where P
1, P
2 represent spin polarizabilities of the respective magnetic layers.

The resistance changing ratio increases as the respective spin polarizabilities increase.
With respect to a relationship between materials for use with ferromagnetic layers
and this resistance changing ratio, ferromagnetic chemical elements of Fe group such
as Fe, Co, Ni and alloys of three kinds thereof have already been reported so far.
[0011] With respect to writing of information in the MRAM, in order to store information
in the selected memory element of the magnetic memory element, this magnetic random
access memory is composed of a plurality of bit write lines, a plurality of word lines
intersecting these bit write lines and TMR elements provided at crossing points between
these bit write lines and word write lines as magnetic memory elements. Then, when
information is written only in the element located at the selected crossing point
of these bit write line and word write line by utilizing an asteroid characteristic
(see Japanese laid-open patent application No.
10-116490, for example).
[0012] The bit write line and the word write line used in that case are made of conductive
thin films such as Cu and A1 which are generally used by semiconductor devices. In
this case, when information is written in a magnetic memory element of which the inverted
magnetic field for generating the above-mentioned inversion of the magnetization is
3183.08 A/m (40 [Oe]), for example, by the bit write line and the word write line,
the bit write line and the word write line being 0.35 µm in width, a current of approximately
10 mA was required. In this case, assuming that the thickness of the write line be
the same as the line width, then a current density required at that time becomes 8.0
x 10
-6A/cm
2. There is then a risk that breaking of wire will be caused by electromigration.
[0013] Accordingly, from a standpoint of the occurrence of electromigration and further
in view of a problem of heat generated by the recording current and from a standpoint
of decreasing a power consumption, this recording current has to be decreased.
[0014] As a means for decreasing the recording current, there is enumerated a method of
decreasing an inverted magnetic field of a TMR element, i.e., coercive force.
[0015] The coercive force of this TMR element is determined based upon the size, shape of
the element, the film arrangement and the selection of the materials. However, although
it is desired that the size of the element should be miniaturized for the purpose
of increasing a recording density of the MRAM, for example, the coercive force of
the element tends to increase due to the miniaturization of the element. Therefore,
the decrease of the coercive force should be attained from the material standpoint.
[0016] If the magnetic characteristic of the magnetic memory element is dispersed at every
element and the magnetic characteristic is dispersed when the same element is used
repeatedly, the selective writing using the asteroid characteristic becomes difficult.
[0017] Therefore, the magnetic memory element is requested to have a magnetic characteristic
by which an ideal asteroid curve can be drawn. In order to draw the ideal asteroid
curve, an R-H (resistance-magnetic field) curve obtained when TMR is measured should
not have noises such as a Barkhausen noise, a rectangle property of a waveform should
be excellent, the magnetization state should be stable and the dispersion of the coercive
force Hc should be small.
[0018] Information may be read out from the magnetic memory element as follows. When magnetic
moments of one ferromagnetic layer and the other ferromagnetic layer across the tunnel
barrier layer are anti-parallel to each other and a resistance value is high, this
state is referred to as a "1", for example. Conversely, when the respective magnetic
moments are parallel to each other and a resistance value is low, this state is referred
to as a "0". Then, information is read out from the magnetic memory element based
upon a difference current obtained at a constant bias voltage or a difference voltage
obtained at a constant bias current in these "1" and "0" states.
[0019] Accordingly, when resistance dispersions between the elements are identical to each
other, a higher TMR ratio (R
max - R
min) R
min where a resistance value R
min represents the low resistance state and a resistance value R
max represents the high resistance state) is advantageous and hence a magnetic memory
device that can operate at a high speed, having a high integration degree and having
a low error rate can be realized.
[0020] A magnetic memory element having a fundamental structure of ferromagnetic layer/tunnel
barrier layer/ferromagnetic layer has a bias voltage dependence of TMR ratio, and
it is known that the TMR ratio decreases as the bias voltage increases.
[0021] When information is read out from the element based upon the difference current or
the difference voltage, it is known that the TMR ratio takes the maximum value of
the read signal at a voltage (Vh) which decreases by half depending upon the bias
voltage dependence. Accordingly, a smaller bias voltage dependence is effective for
decreasing read error in the MRAM.
[0022] Therefore, the TMR element for use with theMRAM should satisfy the above-mentioned
write characteristic requirements and the above-mentioned read characteristic requirements
at the same time.
[0023] However, when the magnetization free layer is generally made of a magnetic material
composed of only ferromagnetic transition metal chemical elements of Co, Fe, Ni, if
the alloy compositions by which the spin polarizabilities shown by P
1 and P
2 in the aforementioned equation (1) are increased are selected, then the coercive
force Hc tends to increase.
[0024] For example, when the magnetization free layer is made of Co
75Fe
25 (atomic %) alloy and the like, although a TMR ratio having large spin polarizabilities
and which is greater than 40% can be maintained, it is unavoidable that the coercive
force also increases. But instead, when the magnetization free layer is made of an
Ni
80Fe
20 (atomic %) alloy which is referred to as a "permalloy" and the like, although the
spin polarizabilities are small as compared with the case in which the magnetization
free layer is made of the Co
75Fe
25 (atomic %) alloy so that the TMR ratio is lowered up to about 33%.
[0025] Further, when the magnetization free layer is made of a Co
90Fe
10 (atomic %) alloy, although a TMR ratio of about 37% can be obtained and its coercive
force can become an intermediate value between the above-mentioned Co
75Fe
25 (atomic %) alloy and Ni
89Fe
20 (atomic %) alloy, this magnetization free layer is inferior in rectangle property
of an R-H loop and an asteroid characteristic by which information can be written
in the element cannot be obtained.
[0026] JP 2001-068760 A has the objective to suppress the reduction in the magnetoresistance effect due to
destruction of a tunnel barrier layer and thereby achieve uniformity and reproducibility.
It is therefore provided an amorphous ferromagnetic layer on at least the interface
of one ferromagnetic layer and the tunnel barrier layer. In claim 5 it is disclosed
that the amorphous ferromagnetic layer is CoFe-X
2, wherein X
2 is chosen from at least one or more kinds of B, Si, C, P, Ti, Zr, Nb, Hf, Mo, Ta,
and W.
[0027] EP-A-1 182 713 A is a prior right which describes a vertical current-type magnetoresistive element.
The element includes an intermediate layer (106) and a pair of magnetic layers (105,
107) sandwiching the intermediate layer, and at least one of a free magnetic layer
(105) and a pinned magnetic layer (107) is a multilayer film including at least one
non-magnetic layer and magnetic layers sandwiching the non-magnetic layer.
[0028] JP 2001-144345 discloses a magnetoresistive effect element which has a magnetoresistance ratio which
depends less on the bias voltage of a ferromagnetic tunnel junction and is high in
serviceability. The magnetoresistive effect element is composed of a ferromagnetic
double tunnel junction, which contains a five-layered structure composed of a ferromagnetic
layer 4, tunnel barrier 5, ferromagnetic layer 6, tunnel barrier 7, and ferromagnetic
layer 8, where tunnel conductance changes with the relative angles of the magnetization
of the three ferromagnetic layers 4, 6, and 8. In the above magnetoresistive effect
device, tunnel conductance increases as an exponential function at a cryogenic temperature
of 4.2 K or so with an increase in a bias voltage of zero or so.
[0029] US 4 236 946 describes a sputtered thin film of an amorphous material composed of a magnetic transition
element X and element Y plus possibly an element Z that has low coercitivity for domains
in the plane, has a well defined and stable magnetic easy axis which is extremely
stable without heating over the Curie point, with a high and flat value of permeability
from low frequencies to greater than 10 megahertz. Metal X can include at least one
of Fe, Ni and Co. Metal Y can include at least one of Si and B. Element Z can be included
composed of Cr, for example.
[0030] EP 0 791 915 A2 discloses a magnetoresistive device of the present invention which includes: a soft
magnetic layer; a hard magnetic layer; a non-magnetic layer formed between the soft
magnetic layer and the hard magnetic layer; and an interface magnetic layer, provided
at an interface between the soft magnetic layer and the non-magnetic layer, for enhancing
magnetic scattering, wherein the soft magnetic layer includes an amorphous structure.
DISCLOSURE OF THE INVENTION
[0031] The present invention is to provide a magnetic memory element having excellent rectangle
property, improved noise and stable magnetic characteristic, improved characteristic
dispersion and excellent asteroid characteristics, the use thereof in a magnetic memory
device whose write characteristics and read characteristics are improved by this magnetic
memory element and methods of manufacturing the magnetic memory element.
[0032] The present invention is directed to a magnetic memory element according to claim
1.
[0033] A magnetoresistive effect element is a magnetoresistive effect element using a ferromagnetic
tunnel junction having a tunnel barrier layer sandwiched between at least a pair of
ferromagnetic layers.
[0034] A magnetization free layer composed of one of the ferromagnetic layers is comprised
of a single layer of a material having an amorphous or microcrystal structure or a
material layer the main portion of which has an amorphous or microcrystal structure.
[0035] This magnetization free layer contains at least two kinds or more than two kinds
of metalloid chemical element and metallic chemical element which are IIIA*(3B)-group
chemical element, IVA*(4B)-group chemical element, VA*(5B)-group chemical element
relative to at least one kind or more than two kinds of components of ferromagnetic
chemical elements of Fe, Co, Ni wherein * ... indicates the CAS notation.
[0036] As the metalloid chemical element and the metallic chemical element, there can be
used two kinds or more than two kinds of B, C, Al, Si, P, Ga, Ge, As, In, Sn, Sb,
Tl, Pb, Bi.
[0037] More preferably, two kinds or more than two kinds of B, Al, Si, Ge should be used
as the metalloid chemical element and the metallic chemical element.
[0038] The metalloid chemical element content and the metallic chemical element content
of this magnetization free layer may be selected within a range of from 5 to 35 atomic
%.
[0039] The magnetization free layer contains at least one kind or more than two kinds of
IVB*(4A)-group chemical element, VB*(5A)-group chemical element on a periodic table
relative to at least one kind or more than two kinds of ferromagnetic chemical elements
of Fe, Co, Ni, wherein *... indicates the CAS notation.
[0040] In this case , as the IVB*(4A)-group chemical element and the VB*(5A)-group chemical
element of the magnetization free layer, there can be used at least one kind or more
than two kinds of Ti, Zr, Nb, Hf, Ta.
[0041] The IVB*(4A) -group chemical element content and the VB*(5A)-group chemical element
content of this magnetization free layer may be selected in a range of from 5 to 25
atomic %.
[0042] Moreover, the magnetization free layer contains at least two kinds or more than two
kinds of metalloid chemical element and metallic chemical element which are IIIA(3B)-group
chemical element, IVA(4B)-group chemical element, VA(5B)-group chemical element on
a periodic table relative to at least one kind or more than two kinds of components
of ferromagnetic chemical elements of Fe, Co, Ni.
[0043] Moreover, in this magnetization free layer, i.e., the magnetization free layer that
contains at least two kinds or more than two kinds of metalloid chemical element and
metallic chemical element which are IIIA(3B)-group chemical element, IVA(4B)-group
chemical element, VA(5B)-group chemical element, on a periodic table and at least
one kind or more than two kinds of IVB(4A)-group chemical element, VB(5A)-group chemical
element on a periodic table relative to at least one kind or more than two kinds of
ferromagnetic chemical elements of Fe, Co, Ni, this magnetization free layer contains
added chemical elements of Cu, N, O, S, the contents of which are selected to be less
than 2 atomic.%.
[0044] Further, in the magnetoresistive effect element, the above-mentioned main portion
of the magnetization free layer is located on the side of the tunnel barrier layer.
[0045] Then, the magnetic memory element according to the present invention is a magnetic
memory element based upon a magnetoresistive effect element using a ferromagnetic
tunnel junction having a tunnel barrier layer sandwiched between at least a pair of
ferromagnetic layers. An information storage layer based upon a magnetization free
layer composed of one of the ferromagnetic layers is comprised of a single layer of
a material having an amorphous or microcrystal structure or a material layer the main
portion of which has an amorphous or microcrystal structure.
[0046] The information storage layer in this magnetic memory element has arrangements similar
to those of the magnetization free layer in the above-mentioned magnetoresistive effect
element.
[0047] Moreover, a magnetic memory device includes a word line and a bit line crossing each
other in a three-dimensional fashion and a magnetic memory element composed of a magnetoresistive
effect element having the above-mentioned respective arrangements of the present invention
located at the portions in which these word lines and bit lines cross each other.
BRIEF DESCRIPTION OF DRAWINGS
[0048]
FIGS. 1A and 1B are respectively cross-sectional views of an example of a magnetoresistive
effect element or a magnetic memory element according to the present invention;
FIG. 2 is a perspective view of a main portion of an example of a magnetic memory
device;
FIG. 3 is a schematic cross-sectional view showing an example of a magnetic memory
element according to the present invention;
FIG. 4A is a schematic plan view of a test element sample of a magnetic memory element;
FIG. 4B is a cross-sectional view taken along the line A - A in FIG. 4A;
FIG. 5A is a diagram of characteristic curves showing a relationship among kinds,
added amounts and coercive forces of IIIA(3B)-group added chemical element to VA(5B)-group
added chemical element in the composition of (Co90Fe10)100-xMx (M represents B, Si, Al, Ge, Mg, Zn) and shows measured results of IIA(2A)-group
Mg and IIB(2B)-group Zn as comparative examples;
FIG. 5B is a diagram of characteristic curves showing a relationship among kinds,
added amounts and TMR ratios of IIIA(3B)-group added chemical element to VA(5B)-group
added chemical element in the composition of (Co90Fe10)100-xMx (M represents B, Si, Al, Ge, Mg, Zn) and shows measured results of IIA(2A)-group
Mg and IIB(2B)-group Zn as comparative examples;
FIG. 6A is a diagram showing a relationship between a composition of a material of
a magnetization free layer and a coercive force measured when Si and two kinds of
B, C, Al, P were added at the same time as the compositions of (Co90Fe10)75Si15M10 (M represents B, C, Al, P);
FIG. 6B is a diagram showing a relationship between a composition of a material of
a magnetization free layer and a TMR ratio measured when Si and two kinds of B, C,
Al, P were added at the same time as the compositions of (CO90Fe10)75Si15M10 (M represents B, C, Al, P) ;
FIG. 7A is a diagram showing a relationship between a composition dependence (B is
added with a constant added amount of 20 atomic %) of a ferromagnetic transition metal
of a magnetization free layer and a coercive force in the composition of (CoxFeyNiz)80B20 and shows measured results obtained when B is not added to the composition as a comparative
example;
FIG. 7B is a diagram showing a relationship between a composition dependence (B is
added with a constant added amount of 20 atomic %) of a ferromagnetic transition metal
of a magnetisation free layer and a TMR ratio in the composition of (CoxFeyNiz)80B20 and shows measured results obtained when B is not added to the composition as a comparative
example;
FIG. 8A is a diagram showing a relationship among added chemical elements, added amounts
and coercive forces of a magnetization free layer material with IVB(4A)-group chemical
element and VB(5A)-group chemical element added in the composition of (Co90Fe10)100-xMx (M represents Ti, Zr, Nb, Ta of IVB(4A)-group chemical element and VB(5A)-group chemical
element) ;
FIG. 8B is a diagram showing a relationship among added chemical elements, added amounts
and TMR ratios of a magnetization free layer material with IVB(4A)-group chemical
element and VB(5A)-group chemical element added in the composition of (Co90Fe10)100-xMx (M represents Ti, Zr, Nb, Ta of IVB(4A)-group chemical element and VB(5A)-group chemical
element) ;
FIG. 9A is a diagram showing a relationship among added chemical elements, added amounts
and coercive forces of a magnetization free layer material into which 10 atomic %
of B, IVB(4A)-group chemical element and VB(5A)-group chemical element were added
at the same time as in the composition of (Co90Fe10)90-xMxB10 (M represents Ti, Zr, Nb, Ta of IVB(4A)-group chemical element and VB(5A)-group chemical
element);
FIG. 9B is a diagram showing a relationship among added chemical elements, added amounts
and TMR ratios of a magnetization free layer material into which 10 atomic % of B,
IVB(4A)-group chemical element and VB(5A)-group chemical element were added at the
same time as in the composition of (Co90Fe10)90-xMxB10 (M represents Ti, Zr, Nb, Ta of 4A-group chemical element and 5A-group chemical element);
FIG. 10A is a diagram showing measured results of a coercive force of a magnetization
free layer in which Cu, Nb, Si, B are added to CoFe at the same time;
FIG. 10B is a diagram showing measured results of a TMR ratio of a magnetization free
layer in which Cu, Nb, Si, B are added to CoFe at the same time;
FIG. 11A is a diagram showing a relationship between a substrate temperature required
when a magnetization free layer is deposited and a TMR ratio;
FIG. 11B is a diagram showing a relationship between a substrate temperature required
when a magnetization free layer is deposited and a TMR ratio;
FIG. 12A is a diagram showing measured coercive forces obtainedwhenamagnetization
free layer has a lamination layer structure composed of a crystal material and an
amorphous material;
FIG. 12B is a diagram showing measured TMR ratios obtained when a magnetization free
layer has a lamination layer structure composed of a crystal material and an amorphous
material;
FIG. 13A is a diagram showing measured values of bias voltage dependences with respect
to TMR ratios in the magnetization free layer according to the present invention;
FIG. 13B is a diagram showing characteristic curves obtained when bias voltage dependences
with respect to TMR ratios in the magnetization free layer according to the present
invention were plotted;
FIG. 14 is a diagram showing resistance versus external magnetic field curves obtained
when a magnetization free layer is composed of (Co90Fe10)80B20 and Co90Fe10;
FIG. 15A is a diagram showing asteroid characteristic curves obtained when a magnetization
free layer is composed of (Co90Fe10)80B20;
FIG. 15B is a diagram showing asteroid characteristic curves obtained when a magnetization
free layer is composed of Co90Fe10; and FIG. 16 is a block diagram showing a magnetic memory device.
BEST MODE FOR CARRYING OUT THE INVENTION
[0049] A magnetoresistive effect element is a magnetoresistive effect element suitable for
use as a magnetic sensor, for example.
[0050] Moreover, a magnetic memory element according to the present invention is a memory
element that can be applied to each memory element of a magnetic memory device.
[0051] Further, a magnetic memory device has an arrangement in which a plurality of bit
write lines (hereinafter referred to as "bit lines" or "BL") and word write lines
(hereinafter referred to as "word lines" or "WL" or "WWL") are crossing each other
in a three-dimensional fashion, magnetic memory elements according to the present
invention being located at crossing points where the bit lines and the word lines
are crossing each other in a three-dimensional fashion.
[0052] First, the fundamental arrangements of the magnetoresistive effect element and the
magnetic memory element according to the present invention are equal to each other,
and therefore these magnetoresistive effect element and magnetic memory element will
be described.
[MAGNETORESISTIVE EFFECT ELEMENT AND MAGNETIC MEMORY ELEMENT]
[0053] A magnetoresistive effect element and a magnetic memory element according to the
present invention have a ferromagnetic tunnel junction structure having a tunnel barrier
layer sandwiched between at least a pair of ferromagnetic layers.
[0054] FIG. 1A is a schematic cross-sectional view of an example of a magnetoresistive effect
element or a magnetic memory element 1 based upon a TMR element having this ferromagnetic
tunnel junction structure. In this embodiment, an underlayer 3 is formed on a substrate,
e.g. Si substrate, and an antiferromagnetic layer 4 is formed on the substrate through
this underlayer 3. A ferromagnetic tunnel junction portion 8 on which a ferromagnetic
layer 5 (hereinafter referred to as a "first ferromagnetic layer"), a tunnel barrier
layer 6 and a ferromagnetic layer 7 (hereinafter referred to as a "second ferromagnetic
layer") are laminated in that order is formed on the antiferromagnetic layer.
[0055] Then, a protective layer 9 which might be called a top-coat layer is formed on this
ferromagnetic tunnel junction portion 8.
[0056] The first ferromagnetic layer 5 is a magnetization fixed layer of which the magnetization
direction is fixed, and the second ferromagnetic layer 7 is a magnetization free layer
of which the magnetization direction is inverted, which is an information storage
layer in the magnetic memory element.
[0057] This magnetization free layer or the second ferromagnetic layer 7 comprising the
information storage layer has an amorphous or microcrystal structure in which the
following alloy chemical elements were added to transition metals (hereinafter referred
to as an "FMTM") of at least one kind or more than two kinds of Fe, Ni, Co.
[0058] Since the magnetization free layer and the information storage layer based upon the
ferromagnetic layer 7 has the amorphous or microcrystal structure as described above
, it can decrease a coercive force while a spin polarizability of the FMTM is being
maintained, it can obtain a soft magnetic characteristic to improve a Barkhausen noise
in an R-H curve and a rectangle property, it can serve as the information storage
layer to decrease dispersions in writing information when the magnetic field is inverted
repeatedly and therefore can obtain satisfactory write characteristics. At the same
time, it can realize a high TMR ratio and can obtain excellent read characteristics
in which a bias dependence characteristic has been improved.
[0059] As chemical elements added to the FMTM that can achieve the above-mentioned effects,
i.e., objects, chemical elements are roughly classified into the following classes
1 to 3.
[0060] Class 1. Addition of metalloid chemical elements and metallic chemical elements of
IIIA(3B)-group chemical elements to VA(5B)-group chemical elements on a periodic table.
[0061] Class 2. Addition of IVB(4A)-group chemical elements and VB(5A)-group chemical elements
on a periodic table.
[0062] Class 3. Addition of either of or both of the chemical elements on the classes 1
and 2 and addition of very small amounts of chemical elements of Cu, 0, N, etc.
[0063] In the magnetoresistive effect element and the magnetic memory element according
to the present invention, the second ferromagnetic layer 7 contains the FMTM that
may contain the alloy-added components shown in the above-described classes 1 and
2 for the purpose of decreasing the coercive force while maintaining the spin polarizability.
Insofar as the above-mentioned objects are achieved, the second ferromagnetic layer
may contain the FMTM and other components than the added components shown on the above-described
classes 1 and 2.
[0064] The above-described class 1 intends to make the magnetization free layer become amorphous.
[0065] Insofar as the above-mentioned objects can be attained, the alloy-based component
may contain more than two kinds of 3B-group and 4B-group metalloids on the periodic
table. As alloy-based components that can be listed in this case, there may be enumerated
a large number of combinations such as FMTM-B-C alloy, FMTM-B-P alloy, FMTM-B-Ge alloy,
FMTM-Si-B alloy, FMTM-Si-P alloy, FMTM-Si-C alloy, FMTM-Si-Al alloy... Of these alloy-based
components, FMTM-Si-B alloy and FMTM-Si-Al alloy should preferably be used as the
above-mentioned alloy-based component.
[0066] The above-described class 2 also intends to achieve effects for improving ability
for making the magnetization free layer become amorphous or improving fine structure
of crystal grains, IVB(4A)-group chemical elements and VB(5A)-group chemical elements
(preferably Ti, Zr, Hf, Nb, Ta) are added to the above-mentioned alloy-based component.
As alloy-based components, there may be listed combinations such as FMTM-Ti alloy,
FMTM-Zr alloy, FMTM-Hf alloy, FMTM-Nb alloy, FMTM-Ta alloy, FMTM-Zr-Nballoy, FMTM-Ta-Nb
alloy, FMTM-Ti-Zr alloy, FMTM-Zr-Ta alloy, FMTM-Zr-Nb-Ta alloy, FMTM-Zr-Nb alloy...
However, of these alloy-based components, there should preferably be listed FMTM-Zr-Nb
alloy, FMTM-Zr-Ta alloy, FMTM-Ta-Nb alloy and the like.
[0067] The above-described class 3 intends to improve ability for making the magnetization
free layer become amorphous or improving fine structure of crystal grains rather than
effects achieved by the metalloids on the classes 1 and 2 and in which the metalloid
chemical elements, the metallic elements and other chemical elements are added to
alloy-based components. As the alloy-based components in this example, there may be
listed innumerable combinations such as ternary alloys such as FMTM-B-Nb alloy, FMTM-B-Zr
alloy, FMTM-Si-Al alloy, FMTM-Si-Nb alloy, FMTM-Si-Zr alloy, quaternary alloys such
as FMTM-Si-B-Al alloy, FMTM-Si-B-Nb alloy... Moreover, main components of chemical
elements added to the FMTM may belong to the above-described classes 1 and 2 and the
above-mentioned alloy-based component may contain other classes such as Cu, 0, N.
Of these alloy-based components, there should preferably be listed FMTM-Si-Al alloy,
FMTM-Zr-B alloy, FMTM-Si-Cu alloy, FMTM-Nb-SiB alloy, FMTM-Si-B-Cu alloy, FMTM-Si-B-Zr-Cu
alloy, FMTM-Si-B-Nb-Cu alloy and the like.
[0068] As described above, when the alloy elements are added to the magnetization free layer
to thereby decrease a coercive force while a spin polarizability for obtaining a large
resistance changing ratio of the information storage layer is being maintained, if
the added chemical elements such as IIIA(3B)-group metalloids to VA(5B)-group metalloids
and IVB(4A)-group chemical elements and VB(5A)-group chemical elements relative to
the FMTM are increased too much, then the amount of the ferromagnetic transition metal
chemical element FMTM decreases excessively so that the film characteristic lost its
ferromagnetism unavoidably. If a resistance value of a target increases too much,
then when this magnetic layer is deposited by a suitable method such as a DC magnetron
sputtering method, it becomes difficult to deposit the magnetic layer, and hence a
trouble arises, in which a film of high quality cannot be deposited.
[0069] In that case, although the cause is not yet clear, troubles arise, in which a magnetic
resistance changing ratio decreases. Therefore, it is to be desired that the added
amounts of metalloid chemical elements and metallic chemical elements (preferably
B, Si, Al, Ge) which are IIIA(3B)-group chemical elements to VA(5B)-group chemical
elements on the periodic table in the case of the class 1 should be less than 50%
although the above-mentioned added amounts may change depending on the composition
of TM.
[0070] If the amount of added chemical elements is too large, then it is frequently observed
that the film characteristic no longer demonstrates its ferromagnetism. Accordingly,
in order to obtain the amorphous or microcrystal system structure, if one kind or
more than two kinds of elements are in use, then it is to be desired that the total
amount of added chemical amounts should fall within a range of from 5 to 35 atomic
%.
[0071] Even when the magnetic layer is given the microcrystal structure, if the chemical
element B is added to the magnetization free layer, then so long as ferromagnetic
deposits such as FeB, Fe
2B, Fe
3B, Co
2B and Co
3B can be obtained, it is to be desired that the added amount of this chemical element
should fall within a range of from 5 to 35 atomic %.
[0072] When IVB(4A)-group chemical element and VB(5A)-group-chemical element (preferably,
Ti, Zr, Hf, Nb, Ta) on the above-described class 2 are added to the magnetization
free layer, if the added amount of these chemical elements is too large, then when
the magnetization free layer cannot have the amorphous structure and loses its ferromagnetism
so that a magnetic characteristic is degraded, thereby lowering a TMR ratio. For these
reasons, it is desirable that the added amount should be about 20 atomic % at most
and that it should be less than the foregoing numerical value.
[0073] When chemical elements on both of the above-described classes 1 and 2 are added to
the magnetization free layer, if the added amount is too large, then the magnetization
free layer loses its ferromagnetism and it becomes difficult to obtain a desired amorphous
structure or a desired microcrystal system as well. Therefore, it is to be desired
that the amounts of these chemical elements added to the FMTM should be less than
approximately 35 atomic % similarly to the case of the IIIA(3B)-group chemical elements
to the VA(5B)-group chemical elements on the class 1.
[0074] So long as the chemical elements on the classes 1 and 2 are both added to the FMTM
and these chemical elements are main components of the added chemical elements , the
magnetization free layer may contain a very small amount of chemical elements such
as Cu, O, S. This will apply for other chemical elements added as well.
[0075] Well-known amorphous and microcrystal soft magnetic materials that are appearing
in the page 298 of "HANDBOOK OF MAGNETIC ENGINEERING written by Kenji Kawanishi, Soshin
Chikazumi, Yoshifumi Sakurai" can be used so long as they meet with the requirements
that have been enumerated so far.
[0076] When the second ferromagnetic layer, i.e., the magnetization free layer or the information
storage layer is comprised of the magnetic material layers having these amorphous
and microcrystal structures, in order to achieve effects for reducing a coercive force
i.e., inverted magnetic field and effects for maintaining a TMR ratio by the amorphous
or microcrystal structure, it is to be desired that this magnetization free layer
or the information storage layer should have a single-layer structure made of this
magnetic material or that most of the main portion of the magnetization free layer
or the information storage layer should be comprised of this magnetic material layer.
[0077] On the other hand, as shown in FIG. 1A, for example, since the magnetization fixed
layer includes the antiferromagnetic material layer 4 which is coupled to the first
ferromagnetic layer 5 in an antiferromagnetic fashion, even when a current magnetic
field for recording information on a magnetic memory, for example, is applied to the
magnetoresistive effect element or the magnetic memory element, the magnetization
direction of the magnetization fixed layer can be prevented from being inverted.
[0078] A ferromagnetic material comprising the first ferromagnetic layer 5 of this magnetization
fixed layer is not limited to some specific ferromagnetic material but an alloy material
composed of one kind or more than two kinds of Fe, Ni, Co can be used as the above
ferromagnetic material.
[0079] Moreover, a material comprising the antiferromagnetic layer 4 may be comprised of
Mn alloy such as Fe, Ni, Pt, Ir, Rh, Co and Ni oxide, etc.
[0080] FIG. 1B shows a schematic cross-sectional view of an example of the magnetoresistive
effect element or the magnetic memory element. As illustrated, the first ferromagnetic
layer 5, i.e. , the magnetization fixed layer can be formed so as to have a lamination
layer ferri structure composed of a first ferromagnetic material layer 51, a non-magnetic
conductive layer 52 and a second ferromagnetic material layer 53.
[0081] Also in this case, the first ferromagnetic material layer 51 is in contact with the
antiferromagnetic layer 4, and hence the magnetization fixed layer 5 is given a strong
magnetic anisotropy of one direction by exchange interaction acting on these two layers.
[0082] The conductive layer 52 in that case can be made of a suitable material such as Ru,
Cu, Cr, Au and As.
[0083] In FIG. 1B, elements and parts identical to those of FIG. 1A are denoted by identical
reference numerals and therefore need not be described.
[0084] A tunnel barrier layer 6 is interposed between the first and second ferromagnetic
layers 5 and 7 shown in FIGS. 1A and 1B as described above. This tunnel barrier layer
lying between the two ferromagnetic layers plays a role not only to break a magnetic
coupling between the first ferromagnetic layer 5, i.e., the magnetization fixed layer
and the magnetization free layer or the information storage layer of the second ferromagnetic
layer 7 but also to cause a tunnel current to flow.
[0085] This tunnel barrier layer 6 can be made of an insulating thin film layer of thin
films of oxide such as A1, Mg, Si, Ca, nitride, halogenide and the like.
[MANUFACTURING METHODS OF MAGNETORESISTIVE EFFECT ELEMENT AND MEMORY ELEMENT]
[0086] Respective layers, i.e., respective magnetic layers and conductive layer comprising
these magnetoresistive effect element and magnetic memory element can be formed by
a vapor deposition method, sputtering, i.e., sputtering vapor deposition method.
[0087] Then, the tunnel barrier layer 6 can be formed by oxidizing or nitriding a metal
film thus formed by sputtering, for example. Alternatively, the tunnel barrier layer
can be formed by a chemical vapor deposition (CVD) method using organic metals, oxygen,
ozone, nitrogen or halogen and halogenated gas.
[0088] The magnetization free layer, e.g. the second ferromagnetic layer 7 comprising the
information recording layer can be manufactured by a vapor-phase growth method such
as a vacuum deposition method, a sputtering vapor deposition method and a CVD (Chemical
Vapor Deposition) method or other suitable method such as electrolytic plating and
nonelectrolytic plating.
[0089] However, when a TMR film has a thickness ranging from several nanometers to several
10s of nanometers as in the case of comprising an MRAM, in general, it is to be desired
that the magnetization free layer or the second ferromagnetic layer should be formed
by a vapor-phase growth method such as sputtering.
[0090] When the magnetization free layer or the second ferromagnetic layer is deposited
by the above-mentioned vapor-phase growth method, for example, if it is deposited
under the condition in which the substrate 2 is not heated, then an amorphous film
can be deposited based upon compositions of materials for depositing the film and
deposition conditions.
[0091] Specifically, when the magnetization free layer based on the second ferromagnetic
layer 7, e.g. information storage layer is formed so as to have an amorphous film
arrangement, since grain boundary does not exist any longer, homogeneity within this
ferromagnetic layer can be improved. Thus, even when the composition ratios of the
FMTM components are equal, the magnetization free layer is formed as the amorphous
magnetization free layer by addition of amorphous chemical elements, thereby making
it possible to decrease a coercive force.
[0092] In that case, in order to deposit the amorphous film, it is to be desired that a
substrate temperature required when the amorphous film is deposited should be kept
under 100°C by a suitable method such as cooling.
[0093] Moreover, there can be used a method for generating finer crystal systems by changing
the film in the form of amorphous state to crystal state. In this case, in order to
demonstrate desired magnetic characteristics, the crystal system should preferably
be made finer and more uniform, and it is desirable that a particle size should be
made under at least 2 nm.
[0094] It is to be desired that a temperature in the heat treatment in that case should
be a temperature higher than approximately a temperature at which the material may
be crystallized and that this temperature should be made lower than a temperature
at which a particle size of deposited microcrystal may be increased by recrystallization.
[0095] A magnetic memory device will be described next.
[MAGNETIC MEMORY DEVICE]
[0096] In a magnetic memory device, a magnetic memory element comprising a memory cell is
comprised of the above-mentioned magnetic memory element 1 according to the present
invention.
[0097] This magnetic memory device can be formed so as to have a cross-point type MRAM array
structure as FIG. 2 shows a perspective view of a schematic arrangement of a main
portion of an example of this magnetic memory device and FIG. 3 shows a schematic
cross-sectional view of one memory cell.
[0098] Specifically, this MRAM includes a plurality of word lines WL arrayed in parallel
to each other and a plurality of bit lines BL arrayed in parallel to each other such
that these bit lines may cross these word lines in a three-dimensional fashion. The
magnetic memory elements 1 according to the present invention are located at portions
in which these word lines WL and these bit lines BL cross each other in a three-dimensional
fashion, memory cells 11 being constructed at these intersecting portions.
[0099] FIG. 2 shows the magnetic memory device at its portion in which 3 x 3 memory cells
are disposed in a matrix fashion.
[0100] FIG. 3 shows a schematic cross-sectional view of this memory cell. In this case,
a switching transistor 13 is formed on a semiconductor substrate 2 composed of a,silicon
substrate, i.e., semiconductor wafer, for example.
[0101] This transistor is comprised of an insulating gate field-effect type transistor,
e.g., MOS transistor. In this case, on the semiconductor substrate 2, there is formed
a gate insulating layer 14 on which an insulating gate portion with a gate electrode
15 deposited thereon is constructed.
[0102] The semiconductor substrate 2 has a source region 16 and a drain region 17 formed
across the insulating gate portion. In this arrangement, the gate electrode 15 constructs
a read word line RWL.
[0103] The semiconductor substrate 2 with this transistor 13 formed thereon has a first
interlayer insulator 31 formed thereon over the gate electrode 15. Contact holes 18
are bored on the respective source region 16 and drain region 17 of the first interlayer
insulator 31 through the interlayer insulator 31, and conductive plugs 19 are filled
into the respective contact holes 18.
[0104] Then, an interconnection layer 20 for the source region 16 is deposited on the first
interlayer insulator 31 over the conductive plug 19 that is brought in contact with
the source region 16.
[0105] Further, a second interlayer insulator 32 is formed on the first interlayer insulator
31 so as to cover the interconnection layer 20.
[0106] The contact hole 18 is bored on the second interlayer insulator 32 over the conductive
plug 19 in contact with the drain region 17, and the conductive plug 19 is filled
into the contact hole.
[0107] A write word line WWL corresponding to the word line WL in FIG. 2 is formed on the
second interlayer insulator 32 along the direction in which the read word line RWL,
for example, extends.
[0108] A third interlayer insulator 33 made of silicon oxide, for example is formed on the
second interlayer insulator 32 so as to cover the write word line WWL. Also in the
third interlayer insulator 33, the contact hole 18 is bored through the conductive
plug 19 that is brought in contact with the drain region 17, and the conductive plug
19 is filled into the contact hole.
[0109] Then, the underlayer 3 made of a conductive material, e.g., Ta is formed on the third
interlayer insulator 33 in contact with the conductive plug 19 that extends through
this third interlayer insulator 33 as shown in FIGS. 1 to 3, for example, and the
magnetic memory element 1 is formed on this underlayer 3.
[0110] Further, a fourth interlayer insulator 34 is formed on the underlayer 3 so as to
cover the magnetic memory element 1, and the bit line BL is formed on this underlayer
insulator across the write word line WL.
[0111] A surface insulating layer is formed on the bit line BL according to the need although
not shown.
[0112] The above-mentioned first to fourth interlayer insulators, the surface insulating
layer and the like can be formed with application of plasma CVD, for example.
[0113] These memory cells 11 are arrayed on the common semiconductor substrate 2, i.e.,
semiconductor wafer in a matrix fashion as shown in FIG. 2.
[0114] Next, the antiferromagnetic layer 4 is regulated in magnetization direction, i.e.,
the antiferromagnetic layer 4 is magnetized in the predetermined direction by a field
anneal treatment, whereby the magnetization of the magnetization fixed layer 5 composed
of a ferromagnetic layer in contact with this antiferromagnetic layer 4 and which
is coupled to this antiferromagnetic layer in an antiferromagnetic fashion can be
fixed to one direction.
[0115] In the magnetic memory device having this arrangement, when a predetermined current
flows to the bit line BL and the write word line WL (WWL), the magnetization direction
of the magnetization free layer is inverted to record information by applying a predetermined
write magnetic field of a synthesized magnetic field of magnetic fields from the two
bit line BL and write word line WL to the magnetoresistive effect element of the memory
cell 11 at the selected intersection point, e.g., the magnetization free layer of
the TMR element 1.
[0116] When information is read out from the magnetic memory device, the transistor 13 is
turned ON by applying a predetermined ON voltage to the gate electrode 15 of the transistor
13 relating to the selected memory cell from which information is read out, i.e.,
the read word line RWL to cause a read current to flow through the bit line BL and
the interconnection layer 20 of the source region 16 of the transistor 13, thereby
resulting in information being read out from the memory cell.
[0117] When the magnetic memory device is manufactured, the aforementioned manufacturing
method can be applied to the magnetic memory element.
[0118] Next, inventive examples will be described. While magnetic memory elements in these
inventive examples are suitable for use with the memory element of the aforementioned
MRAM shown in FIGS. 2 and 3, it is needless to say that they can be applied to magnetic
memory elements in other semiconductor integrated circuits, electronic circuits and
the like.
[Reference EXAMPLE 1]
[0119] A magnetic memory element according to this reference example was formed as a TMR
element including a ferromagnetic tunnel junction portion having a fundamental structure
based upon a lamination layer of the aforementioned ferromagnetic material layer 5/tunnel
barrier layer 6/ferromagnetic material layer 7, i.e., MTJ (Magnetic Tunnel Junction).
[0120] In this case, the first ferromagnetic layer 5 is formed so as to have a lamination
layer ferri structure.
[0121] Moreover, in this case, as in the spin-valve type memory, the ferromagnetic layer
5 is formed as the magnetization fixed layer, of which the magnetization direction
is fixed by the antiferromagnetic layer 4 so that the direction of the magnetization
is constantly set to be constant. The other ferromagnetic layer 7 is formed as the
magnetization free layer, i.e., the information storage layers so that the direction
of the magnetization is inverted with application of external magnetic fields.
[0122] In this reference example, as FIG. 4A shows a plan view of a main portion of the
magnetic memory element and as FIG. 4B shows a cross-sectional view taken along the
line A - A' in FIG. 4A, the switching transistor shown in FIG. 3 and the like were
removed from this magnetic memory element in order to examine magnetoresistive characteristics
of the element.
[0123] In this reference example, first, we have prepared a 0.525 mm-thick Si semiconductor
substrate 2 on which there has been formed a 300 nm-thick insulating layer 12 composed
of a heat oxide film.
[0124] A metal film comprising word lines was formed on the whole surface of this semiconductor
substrate 2, and a word line WL that extends in one direction was formed by pattern-etching
according to photolithography.
[0125] At that time, in the etched portion other than the portion in which the word line
WL is formed, the oxide film of the semiconductor substrate 2, i.e., the insulating
film 12 was etched up to the depth of 5 nm.
[0126] The magnetic memory element (TMR element) 1 was formed on this word line WL. This
TMR element 1 had a lamination layer structure comprised of underlayer 3/antiferromagnetic
layer 4/ferromagnetic material layer 51 of first ferromagnetic layer/conductive layer
52, second ferromagnetic material layer 53/tunnel barrier layer 6/second ferromagnetic
layer 7/protective layer 8, in that order, from below. The arrangement of each layer
has a lamination layer structure comprising Ta (3 nm)/PtMn (30 nm) /Co
90Fe
10 (2 nm)/Ru (0.8)/Co
90Fe
10 (2 nm)/oxide film of Al (1 nm) / (Co
90Fe
10)
100-xMl
x/Ta (5 nm). (In the written form expressing this lamination layer state, a suffix
of each chemical element represents an atomic % and a numerical value within each
parenthesis and which is indicated at the unit of nm represents a film thickness of
each layer. This will apply for the following descriptions as well) .
[0127] The TMR film 1 is composed of a part of this lamination layer film. To this end,
a mask layer (not shown) was formed on the lamination layer film at its portion in
which the TMR element 1 is formed by a photoresist layer, and the pattern of the TMR
element 1 with elliptical flat surface was etched by dry etching using photolithography.
[0128] The pattern of the TMR element 1 in that case had an elliptical shape with a minor
axis of 0.8 µm and a major axis of 1.6 µm.
[0129] Of this film arrangement, other portions than the tunnel barrier layer of the Al
oxide were deposited by a DC magnetron sputtering method. The tunnel barrier layer
of the Al oxide was formed as follows. First, a metal Al film having a thickness of
1 nm was deposited by a DC sputtering system, and the tunnel barrier layer was formed
by plasma-oxidizing a metal Al film with an oxygen : argon flow rate of 1 : 1 at chamber
gas pressure of 0.0133 Pa (0.1 mTorr) by an ICP (inductive Coupled Plasma: inductive
coupled plasma). The oxidation time may change depending upon an ICP output and was
selected to be 30 seconds in this reference example.
[0130] Thereafter, the test sample was annealed within a field anneal furnace with application
of an electric field of 795770 A/m (10 [kOe]) at 270°C for 4 hours, and the magnetization
of the first ferromagnetic layer 5 was fixed to one direction by effecting PtMn regulation
heat treatment on the antiferromagnetic layer 4.
[0131] In this reference example, the composition of CoFe other than the second ferromagnetic
layer 7 comprising the magnetization free layer (information storage layer) was selected
to be Co
90Fe
10 (atomic %). Then, the composition of the second ferromagnetic layer 7 was selected
to be (Co
90Fe
10)
100-xMl
x and in order to contrast the result of this inventive example with a result of Co
90Fe
10 alloy of a comparative example 1 which will be described later on, a ratio of ferromagnetic
transition metal chemical elements of Co and Fe was fixed to Co
90 : Fe
10 and the amount of Ml (B, Si, Al, Ge) was changed from one atomic % to 40 atomic %.
[0132] In the TMR element 1 formed on the above-mentioned substrate 2, as shown in FIG.
4B, an Al
2O
3 insulating layer 30 is treated by sputtering, an opening is formed through the TMR
element 1 by etching using photolithography and a bit line BL extending in one direction
crossing the extending direction of the word line WL is formed over the insulating
layer 30 through this opening by deposition of a metal film and pattern etching using
photolithography.
[0133] Terminal pads 23 and 24 for use in measuring characteristics are formed on each of
both ends of the respective word line WL and bit line BL at the same time the word
line and the bit line are formed.
[REFERENCE EXAMPLE 2]
[0134] In the film arrangement of the TMR element 1, except that the composition of the
second ferromagnetic layer 7, i.e., the magnetization free layer (information storage
layer) was selected to be (Co
90Fe
10)
75Si
15Ml
10 and that Ml was selected to be B, C, P, Al, this reference example had a similar
arrangement to that of the reference example 1.
[Reference EXAMPLE 3]
[0135] In the film arrangement of the TMR element 1, except that the composition of the
second ferromagnetic layer 7, i.e., the magnetization free layer (information storage
layer) was selected to be (Co
90Fe
10)
80B
20, (Co
75Fe
25)
80B
20, (Co
50Fe
50)
80B
20, (Ni
80Fe
20)
80B
20, this reference example had a similar arrangement to that of the reference example
1.
[Reference EXAMPLE 4]
[0136] In the film arrangement of the TMR element 1, except that the composition of the
second ferromagnetic layer 7, i.e., the magnetization free layer (information storage
layer) was selected to be (Co
90Fe
10)
100-xM2
x, M2 was selected to be Ti, Zr, Nb, Ta and that the composition ratio was changed
from 0 to 40 atomic %, this reference example had a similar arrangement to that of
the reference example 1.
[Reference EXAMPLE 5]
[0137] In the film arrangement of the TMR element 1, except that the composition of the
second ferromagnetic layer 7, i.e., the magnetization free layer (information storage
layer) was selected to be (Co
90Fe
10)
90-xB
10M2
x, M2 was selected to be Ti, Zr, Nb, Ta and that the composition ratio was changed
from 0 to 20 atomic %, this reference example had a similar arrangement to that of
the reference example 1.
[INVENTIVE EXAMPLE 1]
[0138] In the film arrangement of the TMR element 1, except that the composition of the
second ferromagnetic layer 7, i.e., the magnetization free layer (information storage
layer) was selected to be (Co
90Fe
10)
73.5Cu
1Nb
3Si
13.5B
9 and (Co
90Fe
10)
73.5Cu
1Nb
3Si
16.5B
6, this inventive example had a similar arrangement to that of the reference example
1.
[Reference EXAMPLE 6]
[0139] In this reference example, the following two samples (1), (2) were manufactured.
In the film arrangement of the TMR element 1, the sample 1 had the composition of
the second ferromagnetic layer 7, i.e., the magnetization free layer (information
storage layer) selected as
[0140] Substrate/Ta (3 nm)/PtMn (30 nm) /Co
90Fe
10 (2 nm) /Ru (0.8 nm) /Co
90Fe
10 (2 nm) /oxide film of Al (1 nm) / (Co
90Fe
10)
80B
20 (2 nm) /Co
90Fe
10 (1 nm)/Ta (5 nm)
[0141] The sample 2 had the above-mentioned composition selected as Substrate/Ta (3 nm)
/PtMn (30 nm)/Co
90Fe
10 (2 nm)/Ru (0.8 nm) /Co
90Fe
10 (2 nm)/oxide film of Al (1 nm) / (Co
90Fe
10)
80B
20 (1 nm)/Co
90Fe
10 (1 nm) / (Co
90Fe
10)
80B
20 (1 nm)/Ta (5 nm)
[0142] Except that the second ferromagnetic layer 7 has the above-mentioned arrangement,
any of these samples (1) and (2) has a similar arrangement to that of the reference
example 1.
[COMPARATIVE EXAMPLE 1]
[0143] In the film arrangement of the TMR element 1, except that the composition of the
second ferromagnetic layer 7, i.e., the magnetization free layer (information storage
layer) was selected to be Co
90Fe
10, Co
75Fe
25, Co
50Fe
50, Ni
80Fe
20, this comparative example had a similar arrangement to that of the reference example
1.
[COMPARATIVE EXAMPLE 2]
[0144] In the film arrangement of the TMR element 1, the composition of the second ferromagnetic
layer 7, i.e. , the magnetization free layer (information storage layer) was selected
to be
[0145] Substrate/Ta (3 nm)/PtMn (30 nm)/Co
90Fe
10 (2 nm)/Ru (0.8 nm) /Co
90Fe
10 (2 nm) /oxide film of Al (1 nm) / (Co
90Fe
10)
100-xM3
x (3 nm)/Ta (5 nm)
[0146] In this film arrangement, the CoFe composition under the tunnel barrier layer other
than the magnetization free layerwas selected to be Co
90Fe
10 (atomic %). With respect to the (Co
90Fe
10)
100-xM3
x, in order to contrast its result with the Co
90Fe
10 alloy of the comparative example 1, a ratio between the ferromagnetic transition
metal chemical elements of Co and Fe was fixed to Co
90Fe
10 (atomic %), the amount of M3 (Mg, Zn) was changed from 1 atomic % to 40 atomic %.
[COMPARATIVE EXAMPLE 3]
[0147] In the film arrangement, the composition of the second ferromagnetic layer 7, i.e.,
magnetization free layer (information storage layer) was selected to be Substrate
/Ta (3 nm)/PtMn (30 nm)/Co
90Fe
10 (2 nm)/Ru (0.8 nm)/Co
90Fe
10 (2 nm)/oxide film of Al (1 nm) / (Co
90Fe
10)
90-xB
10M3
x (3 nm) /Ta (5 nm)
[0148] In this film arrangement, the CoFe composition under the tunnel barrier layer other
than the magnetization free layer was selected to be Co
90Fe
10 (atomic %). This comparative example has a similar arrangement to that of the reference
example 1 except that with respect to the (Co
90Fe
10)
90-xB
10M3
x, in order to contrast its result with the result of the Co
90Fe
10 alloy of the comparative example 1, the ratio between the ferromagnetic transition
metal chemical elements was fixed to Co : Fe = 90 : 10 (atomic %) and the amount of
the M3 (Mg, Zn) was changed from 1 atomic % to 40 atomic %.
[Comparative example 4]
[0149] In the film arrangement of the TMR element 1, this comparative example has a similar
arrangement to that of the reference example 1 except that a magnetization free layer
is composed of a film having a composition of (Co
90Fe
10)
95B
5 and that a substrate temperature required when the magnetization free layer is deposited
was selected in a range of from 50°C to 200°C.
[Comparative example 5]
[0150] In the film arrangement of the TMR element 1, this comparative example has a similar
arrangement to that of the reference example except that the second ferromagnetic
layer 7 has a lamination layer structure such as Substrate/Ta (3 nm)/PtMn (30 nm)/Co
90Fe
10 (2 nm)/Ru (0.8 nm)/Co
90Fe
10 (2 nm)/oxide film of Al (1 nm)/Co
90Fe
10 (2 nm) / (Co
90Fe
10)
80B
20 (1 nm)/Ta (5 nm)
[0151] Characteristics of the above-mentioned reference examples, inventive examples and
comparative examples were evaluated. When the magnetic memory element of the present
invention is used as a memory element of a magnetic memory device, its magnetization
free layer is inverted in magnetization as the information storage layer with application
of a current magnetic field. In this characteristic evaluation, in order to evaluate
the characteristics of the magnetic memory, the magnetization free layer was inverted
in magnetization with application of an external magnetic field and thereby characteristics
were evaluated.
[0152] The TMR element 1 that is used to evaluate magnetic characteristics and TMR ratios
was an ellipse-shaped element having a minor axis of 0.8 µm and a major axis of 1.6
µm.
[0153] A magnetic field for inverting the magnetization of the information recording layer
is applied to the information storage layer in parallel to the easy axis of the magnetization.
An intensity of the magnetic field for this measurement was selected to be 39788.5
A/m (500 [Oe]). At the same time this magnetic field was swept from -39788.5 A/m (-500
[Oe]) to 39788.5 A/m (+500 [Oe]) as seen from one of the east axis of the magnetization
of the information storage layer, the TMR element 1 was conducted in the direction
perpendicular to the film plane by adjusting a bias voltage applied to the terminal
23 of the word line WL and the terminal 24 of the bit line BL such that it might reach
100 mV, and resistance values relative to external magnetic field values and TMR ratios
were measured.
[0154] The TMR ratio was set to (R
max - R
min) /R
min where R
max represents a resistance value obtained in the condition in which the magnetization
of the magnetization fixed layer of the first ferromagnetic layer and the magnetization
of the magnetization free layer (information storage layer) of the second ferromagnetic
layer are anti-parallel to each other and in which the resistance value is high and
R
min represents a resistance value obtained in the condition in which the magnetization
of the magnetization fixed layer and the magnetization of the magnetization free layer
are parallel to each other and in which the resistance value is low.
[0155] A measurement temperature was set to a room temperature of 25°C.
[0156] A coercive force Hc was calculated from a magneto-resistance R - external magnetic
field H characteristic curve that had been calculated from this measurement method.
A crystal structure was observed by a TEM (transmission electron microscope: Transmission
Electron Microscopy). In that case, a crystal structure in which a grain boundary
was not observed from a bright field image of the TEM and in which a halo ring was
observed from an electron beam diffraction figure was determined as an amorphous structure.
[0157] A bias dependence was measured such that, while a bias voltage was changed at the
unit of 100 mV in a range of from 100 to 1000 mV, an R-H loop was measured, a TMR
ratio was calculated and a bias dependence was plotted to the bias voltage.
[0158] Plotted results will be described below.
1. With respect to coercive force and TMR ratio
[0159] TMR ratios and coercive forces of the information storage layers of reference examples
1 to 6, the inventive example 1 and the comparative examples 1 to 5 were evaluated.
Their evaluated results were shown and effects of the present invention will be described.
- [1-1]. In the case in which the magnetization free layer of which the magnetization
is inverted does not contain added chemical element added to FMTM (transition metal)
:
Specifically, the magnetization free layer of the comparative example 1 had a conventional
arrangement in which
Co90Fe10, Co75Fe25, Co50Fe50 Ni80Fe20
[0160] In that case, from observed results obtained by the TEM, it was confirmed that these
materials are of crystal.
TABLE 1
| Composition of magnetization free layer |
Coercive force Hc(Oe)A/m |
TMR ratio (%) |
| Co90Fe10 |
(40) 3183 |
37 |
| Co75Fe25 |
(55) 4376 |
42 |
| Co50Fe50 |
(60) 4774 |
40 |
| Ni80Fe20 |
(25) 1989 |
30 |
[0161] Although the inverted magnetic field Hc of the information storage layer in the TMR
element 1 could be changed depending upon size, shape and thickness of the element,
the size of the element 1 was determined such that the minor axis was fixed to 0.8
µm and the major axis was fixed to 1.6 µm, magnetic material dependences of the TMR
elements 1 in which respective magnetic materials were used to form the magnetization
free layers of the information storage layers were compared with each other.
[0162] Depending upon the structures of word lines and bit lines for generating a current
magnetic field, as the inverted magnetic field of the magnetization free layer of
the TMR element increases, the write current increases. Therefore, reduction of the
inverted magnetic field leads to the decrease of the write current and the decrease
of the power consumption.
[0163] Having compared the coercive force of the magnetic material of the comparative example
1 enumerated on the table 1, Ni
80Fe
20 which might be called a permalloy has the smallest coercive force Hc for influencing
the magnitude of the write current value, and it is to be understood that the write
current value can be suppressed. This permalloy has a TMR ratio of about 30%, which
is small as compared with other materials.
[0164] For this reason, a read output voltage or output current becomes insufficient. On
the other hand, although the Co
75Fe
25 alloy has the largest TMR ratio as compared with these materials, this alloy has
a large coercive force Hc so that write electric power increases. Specifically, it
is to be understood that it is difficult to satisfy the read characteristic and the
write characteristic at the same time.
[0165] When the magnetization free layer comprising the information storage layer is composed
of conventional crystal material, problems arise, in which the CoFe alloy, in particular,
is not excellent in rectangle property of a resistance-magnetic field curve so that
the inverted magnetic field is changed each time it is measured, and therefore is
not stabilized.
[1-2]. Effects achieved when single substances of 3B-group chemical elements to 5B-group
chemical elements are added to the FMTM:
[0166] FIGS. 5A and 5B show measured results of coercive forces Hc and TMR ratios for added
amounts with respect to samples in which the FMTM was fixed to Co : Fe = 90 : 10 in
atomic % and in which B, Si, Al, Ge that are added 3B-group chemical elements to 5B-group
chemical elements were added to this alloy while the added amount was being changed
from 1 to 40% in atomic % and samples having the arrangement of the comparative example
2 and in which Mg and Zn which are other chemical elements than 3B-group chemical
elements to 5B-group chemical elements were added to this alloy while the added amount
was being changed in a range of from 1 to 40% in atomic %.
[0167] In the arrangement in which B, Si, Al, Ge were added to the alloy, as the added amount
increases, the TMR ratio tends to increase temporarily and to be lowered again. Then,
it was confirmed that the inverted magnetic field Hc was lowered by additions of Si,
B, Al, Ge.
[0168] However, although the inverted magnetic field Hc is lowered by addition of Mg of
IIA (2A)-group chemical element, the effects in which the TMR ratios are increased
in each of Si, B, Al, Ge could not be achieved.
[0169] When Zn of IIB (2B)-group chemical element was added to the alloy, neither the TMR
ratio could be increased nor the inverted magnetic field Hc could be decreased.
[0170] Specifically, according to the arrangement in which these IIA (2A)-group chemical
element and IIB (2B)-group chemical element are added, the increase of the TMR ratio
and the decrease of the inverted magnetic field, i.e. , the read characteristic and
the write characteristic are not compatible each other and the above-mentioned alloy
is not suitable for as the material of the magnetization free layer of the information
storage layer in a magnetic memory element.
[0171] While the effects achieved when B, Si, Al, Ge were added as the IIIA (3B)-group chemical
element to VA (5B)-group chemical element are shown in the above-mentioned reference
examples of the present invention, it is supposed that similar effects could be achieved
with respect to C, P, Ga, In, As, Se, Sn, Sb, Te located near B, Al, Ge in a periodic
table and whose features are similar, other metalloid chemical elements and IIIA (3B)-group
and IVA (4B)-group metallic chemical elements.
[0172] As described above, while B, Si, Al, Ge and the IIIA (3B)-group to VA (5B)-group
metalloid chemical elements and metallic chemical elements located around these chemical
elements in the periodic table and of which features are similar can achieve effects
for improving TMR ratios and decreasing coercive forces, of these chemical elements,
chemical elements such as B, Si, P, Al, Ge are particularly desirable.
[0173] From the results shown in FIGS. 5A and 5B, when the added amounts of these chemical
elements are too small, the effects for improving TMR ratios are small and effects
for decreasing coercive forces are small. If the aforementioned effects are achieved,
then at least more than 5 atomic % of the IIIA (3B)-group to VA (5B)-group metalloid
and metallic chemical elements should be added. If the added amount is too large,
then although some added chemical element having an added amount of 40 atomic % can
continue the coercive fore to decrease, the magnetization amount decreases too much.
As a result, there is a risk that the TMR ratio will decrease. Even when the added
amount exceeds 35%, there can be achieved the effect that the magnitude of the coercive
force Hc will decrease. However, in order to make the low coercive force become compatible
with a high TMR ratio, it is to be desired that the added amount should not exceed
35%. Therefore, it is to be desired that the most suitable added amount of the added
chemical element that can improve the TMR ratio and make it and the coercive force
become compatible with each other should fall within a range of from 5 to 35 atomic
% when one chemical element is added to the FMTM.
[0174] Having observed TEM images of the cross sections of the magnetization free layer
having the composition of the (Co
90Fe
10)
80B
20 of the reference example in which the coercive force could be decreased and of the
magnetization free layer having the composition of the (Co
90Fe
10)
97B
3 of the comparative example in which the effect for decreasing the coercive force
is small, it is to be understood that the fine structure of the (Co
90Fe
10)
80B
20 is an amorphous layer and the fine structure of the (Co
90Fe
10)
97B
3 is microcrystal. It is considered that the coercive force Hc can be decreased because
the fine structure is the microcrystal and amorphous layer.
[0175] As will be described in the magnetization decision behavior item that will be described
later on, since the fine structure is the amorphous layer, the rectangle property
of the resistance-magnetic field curve can be improved, the behavior of the magnetization
inversion can be stabilized, and the dispersions of the magnetization inversion can
be decreased. From this standpoint, when the magnetization free layer is formed of
the amorphous ferromagnetic material, the read characteristics can be improved, and
therefore the amorphous ferromagnetic material is the suitable material as the magnetization
free layer.
[1-3]. Effects achieved by addition of more than two kinds of IIIA (3B)-group to VA
(5B)-group chemical elements:
[0176] The effect for increasing the TMR ratio and the effect for decreasing the coercive
force can be achieved only when only one kind of IIIA (3B)-group to VA (5B)-group
metalloid chemical elements is contained but also when more than two kinds of them
are contained.
[0177] The arrangement of the reference example 2 contains more than two kinds of these
chemical elements. FIGS. 6A and 6B show results obtained when Si was selected as the
first added chemical element, the added amount was selected to be 15 atomic % and
B, C, P, Al were added as the second added chemical elements. Even when the suitable
material contains more than two kinds of these chemical elements, it can be recognized
that the coercive force Hc can be decreased and the TMR ratio can be increased as
has been described in the above-described [1-2]. In particular, when Si, B and Si,
Al are added at the same time, the coercive force Hc can be decreased remarkably.
[0178] As described above, the TMR ratio can be increased and the coercive force can be
decreased when the arrangement of the present invention contains two kinds of IIIA
(3B)-group to VA (5B)-group metalloid chemical elements and metallic chemical elements.
[0179] Moreover, it is to be considered that similar effects can be achieved even when the
arrangement of the present invention contains more than three kinds of IIIA (3B)-group
to VA (5B)-group metalloid chemical elements and metallic chemical elements.
[0180] Therefore, IIIA (3B)-group to VA (5B)-group chemical elements are not limited in
particular, and two kinds or more than two kinds should preferably be selected from
B, C, Si, P, Al.
[1-4]. Composition dependence of ferromagnetic transition metal chemical elements
obtained when 20 atomic % of B is added to the arrangement of the present invention:
[0181] Of the magnetization free layer material in which chemical elements were added to
make the magnetization free layer become amorphous, with respect to the composition
ratios of Fe, Co, Ni which are ferromagnetic chemical elements and TMR ratios and
values of coercive force Hc, effects will be described with reference to measured
results of a sample in which 20 atomic % of B in the reference example 3 was added
and a sample that does not use the added chemical elements of the comparative example
1.
[0182] FIGS. 7A and 7B show measured results of the reference example 3 and the comparative
example 1 altogether. In the sample in which B that is IIIA (3B)-group to VA (5B)-group
chemical elements is added, the composition ratio of any ferromagnetic transition
metal of Co
90Fe
10, Co
75Fe
25, Co
50Fe
50, Ni
80Fe
20 can increase the TMR ratio and decrease the coercive force Hc as shown in the reference
example 1 of the aforementioned [1-2].
[0183] Therefore, these effects are not limited to the compositions of CoFe, NiFe, and such
effects can be achieved with respect to a magnetic memory element including an alloy-based
magnetization free layer in which approximately 5 to 35 atomic % of Al which is one
of IIIA (3B)-group to VA (5B)-group metalloid chemical elements are added to Fe, Co,
Ni having any composition range.
[0184] Moreover, with respect to the added chemical elements, the arrangement may contain
not only N shown herein but also IIIA (3B)-group to VA (5B)-group metalloid and metallic
chemical elements and Al or the added chemical elements that will be described later
on.
[1-5]. Effects achieved by addition of one kind of IVB (4A)-group and VB (5A)-group
chemical elements:
[0185] FIGS. 8A and 8B show composition dependences of coercive forces Hc and TMR ratios
obtained when Ti, Zr, Nb, Ta of so-called bubble metals of IVB (4A)-group and VB (5A)-group
metals are added to the FMTM in the sample having the arrangement of the reference
example 4.
[0186] The coercive force Hc can be decreased by the addition of these chemical elements.
With respect to the sample with the added amount of 15 atomic % in which the coercive
force Hc can be decreased through the TEM observation in which FMTM-Zr alloy was used
in the magnetization free layer, it is to be understood that this sample has the amorphous
layer. On the other hand, with the added amount of 3 atomic %, the effect for decreasing
the coercive force Hc is small. It is considered that the reason for this is based
upon the effect for making the sample become amorphous or making the crystal grain
become fine. The coercive force Hc can be decreased in Ta, Zr, Nb as described above,
and similar effects can be achieved in so-called bubble metals of IVB (4A)-group and
VB (5A)-group metals. Although the added amount is not limited in particular so long
as the above-mentioned effect can be achieved, from the experimental results shown
in FIGS. 8A and 8B, the added amount should preferably be selected to be approximately
25 atomic % at the most in a range in which a satisfactory TMR ratio can be obtained
and the coercive force Hc can be decreased. It is needless to say that similar effects
can be achieved not only when these added chemical elements are solely added to the
FMTM but also at least one kind or more than two kinds of these added chemical elements
are contained in the samples.
[1-6] . Effects achieved when IIIA (3B)-group to VA (5B)-group chemical elements and
IVB (4A)-group and VB (5A)-group chemical elements are added to the samples:
[0187] FIGS. 9A and 9B show characteristic evaluation results obtained when 10 atomic %
of B is added to the TMTM and Ti, Zr, Nb, Ta are contained in the sample of the reference
example 5. Having compared with the effects achieved by the addition of the IIIA (3B)-group
to VA (5B)-group chemical elements in the reference example 1, it is to be noted that,
if these chemical elements are further added, the coercive force can be further decreased
although the effects are small while the high TMR ratio obtained by the IIIA (3B)-group
to VA (5B)-group chemical elements is being maintained. It is needless to say that
these effects are not limited to Ti, Zr, nb, Ta and it can be easily estimated that
such effects can be achieved in Hf, v which are the IVB (4A)-group to VB (5A)-group
chemical elements that belong to the same groups in the periodic table.
[1-7]. Multinary system:
[0188] If the effects shown by the measured results of the TMR ratio and the coercive fore
Hc are achieved, the arrangements of the reference examples 1 to 5 should contain
the above-mentioned IIIA (3B)-group to VA (5B)-group chemical elements and the IVB
(4A)-group to VB (5A)-group chemical elements , these arrangements may contain trace
element of minute amount in addition to the above-mentioned chemical elements.
[0189] FIGS. 10A and 10B show evaluated results obtained by the arrangements of the inventive
example 1 and the comparative example 1. As illustrated, even the system which contains
Cu in addition to the chemical elements that have been shown so far can decrease the
coercive force Hc and can improve the TMR ratio.
[1-8]. Substrate temperature obtained when magnetization free layer is deposited:
[0190] FIGS. 11A and 11B show the coercive force Hc and the TMR ratio relative to the substrate
temperature with respect to the sample having the arrangement of the comparative example
4 in which effects of substrate temperatures obtained when the magnetization free
layer is deposited have been examined. From the standpoint of conditions in which
the amorphous layer is formed, the process for forming the magnetization free layer
by heating the substrate exerts a bad influence upon the decrease of the coercive
force Hc and the improvement of the TMR ratio that have been mentioned so far, and
the result in which the magnetization free layer is deposited at room temperature
is most excellent. Accordingly, from the view point of forming the amorphous structure,
it is not preferable that the substrate is heated when the magnetization free layer
is deposited. Hence, the substrate temperature should be at least less than 100°C
and the substrate should preferably be cooled.
[1-9]. Lamination layer structure:
[0191] FIGS. 12A and 12B show measured results of magnetization free layer materials, the
coercive forces Hc and the TMR ratios obtained when the magnetization free layers
of the inventive example 1 and the comparative example 5 are formed so as to have
lamination layer structures.
[0192] Coercive forces can be decreased and high TMR ratio can be achieved similarly by
the magnetization free layers based on the lamination layer structure of the amorphous
layer formed by the addition of two kinds or more than two kinds of IIIA (3B)-group
to VA (5B)-group chemical element metalloid and metallic chemical elements on the
periodic table and the crystal layer. In this case, although the cause is not yet
clear, the amorphous layer should preferably be used for the side of the tunnel barrier
layer. When the crystal layer is laid adjacent to the side of the tunnel barrier layer,
as shown in FIG. 11 in the comparative example 4, the decrease of the coercive force
was not recognized.
2. Bias dependence:
[0193] FIGS. 13A and 13B show bias voltage dependences of TMR ratios obtained when the magnetization
free layer is formed of the Co
90Fe
10 alloy of the comparative example 1 and the magnetization free layer is formed of
the (C0
90Fe
10)
80B
20.
[0194] FIG. 13A shows the bias voltage dependences in the form of measured values, and FIG.
13B is a graph in which these measured values are plotted. Although the cause is not
yet clear at present, when the magnetization free layer of the present invention is
in use as illustrated, the bias dependence can be improved, the output characteristic
at real operation bias voltage can be improved so that it becomes easy to discriminate
the low-resistance state and the high-resistance state. As a result, the read characteristic
of the magnetic memory element can be improved.
3. Magnetization inversion behavior:
[0195] Similarly in FIG. 14, a resistance-external magnetic field curve obtained when the
magnetization free layer is formed of the (Co
90Fe
10)
80B
20 of the reference example 1 and a resistance-external magnetic field curve obtained
when the magnetization free layer is formed of the Co
90Fe
10 alloy of the comparative example 1 are shown by curves 40 and 41, respectively. As
described above, when the information storage layer of the present invention is used,
the coercive force Hc can be decreased while the high TMR ratio can be maintained.
Moreover, the rectangle property of the R-H loop can be improved, and the Barkhausen
noise also can be decreased. As a result, not only the write current can be decreased
but also the shape of the asteroid curve can be improved and hence the write characteristic
can be improved, thereby making it possible to decrease the write error.
[0196] FIGS. 15A and 15B show measured results obtained when asteroid curves of 20 elements
have been overlapped. FIG. 15A shows measured result when the magnetization free layer
is made of (Co
90Fe
10)
80B
20 and FIG. 15B shows measured results when the magnetization free layer is made of
Co
90Fe
10. As is clear from the results obtained when FIGS. 15A and 15B have been compared
with each other, it is to be understood that, when the magnetization free layer is
formed of Co
90Fe
10 which is the conventional crystal material, most of the asteroid curves is deviated
from the ideal asteroid shape. Hence, this magnetic memory is inferior in read characteristic.
However, when the magnetization free layer is made of the amorphous ferromagnetic
material of the present invention, the asteroid shape can become ideal and can be
stabilized.
[0197] This effect can be achieved not only when the memory element uses the magnetization
free layer having the material composition shown in FIG. 15 but also when the amorphous
ferromagnetic material in the range of the present invention is used in the main portion
of the magnetization free layer. Therefore, according to the present invention, the
write characteristic to the memory element can be improved considerably, and the write
error of the MRAM can be decreased.
[0198] Next, a specific circuit arrangement of an example of a magnetic memory device MRAM
will be described with reference to FIG. 16 which shows a block diagram of a circuit
arrangement. This MRAM comprises a cell array portion 160 formed by the array of memory
cells 11 and a marginal circuit portion 161.
[0199] The cell array portion 160 comprises a plurality of memory cells 11 arranged in rows
and columns. Each memory element includes a memory element 1 composed of MTJ and a
transistor 13 that can select the cell.
[0200] The marginal circuit portion 161 includes decoders 162, 163 for selecting the cell
from address information, drivers 164, 165 for causing a write current to flow, a
sense amplifier 166 for selecting a read current and the like.
[0201] Then, the marginal circuit portion 161 includes a bit line BL, a write word line
WWL and a read word line RWL, each of which is extended to the cell array portion
160. The bit line BL is connected to the decoder 162, and each memory cell 11 is accessed
through the bit line BL.
[0202] Write operations, read operations in this magnetic memory device MRAM and respective
arrangements thereof will be described.
[Write operation]
[0203] In order to write information in the memory cell 11, it is necessary to use a magnetic
field generated by a current. The lines BL and WWL are interconnections necessary
for causing a current to flow. The lines BL and WWL are located so as to cross each
other in the upper and lower direction across the memory cell as mentioned hereinbefore.
The drivers (inverters) 164 and 165 for applying a write current are connected to
both ends of the lines BL and WWL. The gates of the drivers are connected to the decoders
162 and 163 for converting address data inputted from the outside and select the lines
BL and WWL to which the write current should be applied.
[0204] In the line BL for generating the inverted magnetic field for inverting the magnetization
direction of the information storage layer 7 of the memory element, i.e. , magnetoresistive
effect element, the direction of the write current, i. e. , the information write
current of "0" or "1" may be controlled based upon the data line input. On the other
hand, in the line WWL for generating an assist magnetic field, although the direction
of the write current may be constant, considering the electromigration, the direction
in which the current flows can be inverted each time information is written in the
information storage layer.
[Read operation]
[0205] The lines BL and RWL are used to read information from the memory cell in which information
of "0" and "1" have been written as described above. A cell from which information
is to be read out may be selected by a transistor 13 provided in each memory cell.
The gate of the transistor is connected to the line RWL and the drain is connected
to one end of the MTJ, respectively. Then, the other end of the MTJ is connected to
the line BL. The lines BL and RWL are connected to the decoder and the lines BL and
RWL thus selected for reading are alerted. A sense current may flow to the thus selected
cell through the channel of the line BL, the MTJ and the transistor, and the magnitude
of the sense current is detected by a sense amplifier 166. Specifically, "0" and "1"
of recorded information may be discriminated from each other, i.e., recorded information
may be read out from the memory cell.
[0206] In the magnetoresistive effect element in a magnetic sensor or the like, the magnetic
memory element in the magnetic memory device according to the present invention that
have been described so far, when the magnetization free layer is composed of a single
layer of an amorphous or microcrystal material or the main portion of the magnetization
free layer is composed of the amorphous or microcrystal material, the single layer
of or the main portion of the magnetization free layer is composed of the magnetic
material in which two kinds or more than two kinds of IIIA (3B)-group, IVA (4B)-group
and VA (5B)-group chemical elements and at least one kind or more than two kinds IVB
(4A)-group and VB (5A)-group chemical elements are added to at least one kind or more
than two kinds of ferromagnetic transition metal chemical elements Fe, Co, Ni on the
periodic table.
[0207] According to this arrangement, as is clear from the above descriptions, in the magnetoresistive
effect element, the rectangle property in the R-H characteristic may be made excellent
and the noise may be decreased. Hence, this magnetoresistive effect element is suitable
for use as magnetic sensors for various applications such as a magnetic detector and
a magnetic head.
[0208] Moreover, in the magnetic memory element and the magnetic memory device, the read
signal can be increased by increasing the TMR ratio, and the write current can be
decreased. Further, when information is read out from the magnetic memory element
or the magnetic memory device, the bias dependence characteristic of the TMR ratio
can be improved and then low-resistance state and the high-resistance state can be
discriminated from each other with ease, thereby resulting in the read characteristic
being improved. When information is written in the magnetic memory element or the
magnetic memory device, the noise in the resistance-external magnetic field curve
can be improved and the write error can be decreased. Specifically, both of the write
characteristic and the read characteristic can be satisfied.